Optical fiber and method of producing

ABSTRACT

A starting material for producing optical fibers contains metal halides. The refractive index of the optical fiber formed from the starting material is predeterminable by adjusting a partial pressure ratio of a halogen-containing gas mixture. The starting material is produced by mixing halogenated gases into a gas mixture with the desired partial pressure ratio, causing a chemical reaction at a first temperature of the gas mixture with at least metal to form a reaction product, the first temperature being higher than the melting temperature of the reaction product and cooling the reaction product to a second temperature that is below the melting temperature.

[0001] This application is a divisional of U.S. patent application Ser.No. 09/944,825, now U.S. Pat. No. 6,564,587, dated May 20, 2003.

[0002] The present invention relates to an optical fiber and a processfor producing the optical fiber, especially an optical fiber havingproperties surpassing those known in the prior art.

BACKGROUND OF THE ART

[0003] Predominantly metal halides are used for radiation conductionwith optical fibers in the medium infrared spectral range, which coversthe wavelength range between approx. 4 and 18 micrometers. One isdealing in this connection with polycrystalline materials as a rule.

[0004] Known fibers have high leakage based on a relatively roughstructure and numerous impurities and the fibers' low mechanical loadcapacity.

[0005] Optical fibers normally have an fiber-optic channel or core and acladding with a refractive index n that deviates from that of the core,in particular, usually being lower than that of the core. A light wavethat is coupled into the core of the fiber is ideally fully reflectedbetween the core and the cladding and held in the optical fiber in thismanner. The cladding is primarily supposed to prevent the overflow oflight, for example, from one core to another in a bundle of fibers.

[0006] A special type of optical fibers are so-called single modefibers, which fulfill special known conditions as such with respect tothe size of the core diameter with reference to the ratio of wavelengthsto be coupled to the numeric aperture. These types of single-mode fibershave extraordinarily high requirements and are used for example for theheterodyne detection of objects, whereby the radiation emanated from theobject of a specific wavelength is coupled into two laterally separatedsingle-mode fibers and the phase or time displacement between the twofibers is evaluated from the signals picked up on their respective ends.

[0007] Another special type of optical fibers is represented by theso-called SELFOC fibers, which are self-focusing. Self-focusing meansthat an image coupled into such a fiber in one location recurs atcertain intervals similar to the situation with a sequence of convergentlenses, which are at such intervals from one another that the focalpoint corresponds at both sides of the convergent lenses with one of thefocal points of the next respective convergent lens. A parabola-likeindex of refraction profile of the optical fibers is required in thisconnection. As a result, an object of the present invention is toprovide a process for producing an optical fiber with which high productquality can be reliably. In addition, it is an objective of theinvention to disclose an optical fiber with the best possiblefiber-optical characteristics, in particular in the medium infraredspectral range.

SUMMARY OF THE INVENTION

[0008] The objective is attained with respect to the process aspect forone by a process to produce a starting material containing metal halideswith a specific index of refraction for an optical fiber with thefollowing steps:

[0009] Mixing halogenated gases into a gas mixture with a partialpressure ratio that is a function of the index of refraction of thestarting material,

[0010] Causing a chemical reaction of the gas mixture with one metal toat least one reaction product with an initial temperature above themelting temperature of the reaction product and.

[0011] Cooling the reaction product to a second temperature below themelting temperature.

[0012] In accordance with the invention, halogenated gases are firstmixed. Then a direct chemical reaction between the halogen particles anda metal or a metallic mixture is brought about.

[0013] The mixing ratio of the halogenated gases is selected inaccordance with the index of refraction desired for the startingmaterial containing metal halides that is being produced. Any index ofrefraction can be set with the process in accordance with the inventiondue to the adjustable mixing ratio of the halogenated gases within avalue interval prescribed by the respective pure metal halides.

[0014] Thus, silver halide has an index of refraction of approx. 2 inthe spectral range between 4 and 14 micrometers, for example.

[0015] In many embodiments, the correct mixing ratio be attained byadjusting the partial pressures of the halogenated gases that are used.The partial pressure ratio can be adjusted, for example, bycorrespondingly controlling the opening of the gas valves at the outletof the gas containers each of which contains one of the halogenatedgases. Alternatively, an individual gas source in which the halogenatedgases are already present in the required mixing ratio can be used inthe production process.

[0016] The correct partial pressure ratio is set as a function of thedesired index of refraction in accordance with the boundary conditionsof the chemical reactions being caused. In this case, the halogensinvolved in the reaction, the metal or metals involved in the reaction,the reaction temperature and the reaction atmosphere (inert gas orvacuum, for example) can influence the setting of the partial pressureratio.

[0017] The process in accordance with the invention overcomes thelimitation that exists with known production processes of the mixingratio of metal halides in the starting material being limited to a verylimited value interval.

[0018] In the case of one embodiment of the invention, the reaction ofthe halogen particles with the metal or the metal mixture is broughtabout in a vacuum. Alternatively, the chemical reaction can take placein an inert gas atmosphere.

[0019] In at least one embodiment, the inventive process is designed toproduce a solid solution of metal halides.

[0020] In these embodiments, alkali metals, in particular potassium,sodium or cesium, rubidium or thallium or silver are used as metals.

[0021] Gases containing bromine, iodine or chlorine are used ashalogenated gases individually or in combination in different exemplaryembodiments. Halogen gases with especially high purity are typicallyused. Commercially available high-purity halogen gases can be used forthis or correspondingly designed purity steps can be added to theproduction process itself.

[0022] The process in accordance with the invention is suitable inparticular for producing a solid solution of AgBr_(x)C_(1-x) over theentire range of the mixing ratio, i.e. 0≦x≦1. This starting material foroptical fibers can be produced with the process in accordance with theinvention with especially high mechanical ruggedness and opticalquality.

[0023] The partial pressure ratio is set in another embodiment of theinvention in such a way that the solid solution contains bromine andchlorine in a particle number ratio of 3 to 1.

[0024] The microstructure of the polycrystalline solid solution isespecially homogenous with this ratio. As a result, the light scatter inthe fibers is minimized.

[0025] In another embodiment of the process in accordance with theinvention, the metal is purified electrolytically in an additional stepbefore the chemical reaction with the halogens is brought about.

[0026] In order to produce especially pure starting material for opticalfibers, the liquid reaction product is guided through a purificationstage before the step of cooling to a temperature below the meltingpoint. Plans can be made for several consecutive purification steps. Thepurification takes place by guiding the liquid reaction product throughcapillary vessels, for example.

[0027] Another purification effect is achieved in an exemplaryembodiment by moving the reaction product along a temperature gradientin a furnace during cooling from the first temperature to the secondtemperature. A temperature gradient can be set for example in a reactorwith an oblong furnace by providing heating elements that can becontrolled separately along its longitudinal extension. Thus, thereaction product can be cooled bit by bit, wherein the crystallizationfront is stationary. The crystallization front is the area within thereactor in which the reaction production falls short of the meltingtemperature and crystallizes.

[0028] Another inventive idea independently worthy of protectionconcerns a process to produce a blank for optical fibers with thefollowing steps:

[0029] Preparing a bath with liquid starting material,

[0030] Rotating a solid core that is partially submerged in the bath insuch a way that a thin layer of the starting material accumulates on thecircumferential surface of the core in such a way and crystallizes thereso that the solid core grows in the radial direction while rotating.

[0031] In the case of the process in accordance with the invention,first a bath is prepared with the starting material. This can beaccomplished for example using the process steps from the processdescribed above, i.e.:

[0032] Mixing halogenated gases into a gas mixture with a partialpressure ratio that is a function of the index of refraction of thestarting material,

[0033] Causing a chemical reaction of the gas mixture with one metal toat least one reaction product with an initial temperature above themelting temperature of the reaction product.

[0034] The liquid reaction product is then collected in a bath and keptthere at a temperature above the melting point. For this purpose,heating elements can be built into the walls of a vessel in which thebath is situated, for example.

[0035] Basically, other known processes can also be used to produceliquid starting material, however.

[0036] Liquid starting material can be refilled continuously or meteredout step by step during the subsequent process steps. If a secondstarting material is refilled, the index of refraction of thecrystallizing material changes in accordance with the concentration ofthe second starting material. An index of refraction gradient can becreated in the radial direction in this manner.

[0037] Regardless of whether the refilled starting material remains thesame during the production process or another starting material isrefilled, as well as regardless of whether the refilling takes placecontinuously or in separate batches, one embodiment has means tohomogenize the liquid starting material in the bath. These homogenizingmeans can be designed, for example, so that they regularly orirregularly set the bath into vibration. Thus, a piezoelectric vibrationgenerator is provided, which is connected with a tub for the bath of theliquid starting material. As an alternative or in addition to this, gaslines can be provided along the bath, which having openings distributeduniformly along their length from which gas can exit. The gas bubblesascending in the bath move the liquid starting material and therebyblend it together in this way.

[0038] In the process in accordance with the invention, a solid core isthen partially submerged in the bath. The core is composed for exampleof the same material as the bath. A homogenous blank can be produced inthis way.

[0039] Using a core that has the bath material only on itscircumferential surface and an inside core of second material is alsoconceivable. A blank with the shape of a hollow cylinder can be producedthis way by subsequently removing the inside core.

[0040] Finally, the core can also be composed completely of anothermaterial than the bath. A blank with a core and cladding can be producedin this way by crystallizing the bath material on the core. Tthe coreand cladding should have different optical properties.

[0041] For example, a core can be used that is composed of a solidsolution of AgBr and AgCl with a first mixing ratio. Due to thecrystallization of the liquid starting material, which has anothermixing ratio than that of the core, a blank is formed with a cylindricalshape, for example, whose core and cladding have different indices ofrefraction.

[0042] Rotating the core takes place in such a way that a thin layer ofthe starting material accumulates on the circumferential surface of thecore and crystallizes there. The crystallization takes place by coolingthe liquid material adhering to the circumferential surface in contactwith an inert gas atmosphere or in a vacuum after re-emerging from thebath.

[0043] The rotating speed of the core is set in such a manner that anoptimum is achieved with respect to the growth speed, on the one hand,and with respect to crystal quality, on the other. The grown materialshould have a homogeneous microstructure and cause only low leakage.

[0044] The growth on the circumferential surface takes place, as seen asa whole, in a radial direction, i.e., perpendicular to the rotationalaxis. Of course, this does not preclude in particular a crystal bond ofadhering particles from also occurring on neighboring, previouslycrystallized areas in the circumferential direction.

[0045] Depending upon the temperature of the bath and reactionatmosphere, the crystallization of adhering liquid material can takeplace directly after emergence from the bath or at a later point in timebefore the next re-submersion in the bath.

[0046] The process in accordance with the invention is especially suitedfor producing cylindrical blanks for optical fibers. Other geometricshape can be realized in principle, however. For example, by usinginfrared irradiation on limited sections of the surface along therotational axis of the growing blank outside the bath, crystallizationcan be prevented in these areas. In this way, a non-homogenous crystalgrowth is created in the radial direction along the rotational axis.Using targeted irradiation, for example by using correspondinglyinstalled projection lenses for the irradiated infrared light, blankscan be realized with any geometric shape, as a rule. The shape will havecylindrical symmetry if the radiation is constant in terms of time, and,if the radiation is varied in terms of time, other shapes can also berealized.

[0047] In one embodiment of the invention, the liquid staring materialis replaced in the bath while rotating the core by another startingmaterial for another index of refraction. Blanks can be produced in thisway with a sequence of different material layers in the radialdirection. For example, layers with difference indices of refraction canfollow one another in the radial direction. The material layers in thisembodiment have relatively sharp boundaries so that the index ofrefraction changes in a stepped manner in the radial direction.

[0048] A continuous variation of the material properties can be attainedby continuously exchanging the liquid starting material in the bathwhile rotating the core. Thus, it is possible to continuously increasethe concentration of AgBr in an AgCl bath via an inflow of pure AgBr. Aliquid AgBr/AgCl solution with a relatively high concentration of AgBrrelative to the bath can also be used instead of pure AgBr.

[0049] To produce cylindrical blanks, the process is conducted so thatthe rotational axis always runs parallel to the surface of the liquidstarting material.

[0050] It is typical that the distance between the rotational axis andthe surface of the liquid starting material increases continuously. Thisis accomplished while the submersion depth of the growing blank remainsconstant during growth, so that there are always constant growthparameters.

[0051] Another inventive idea independently worthy of protectionconcerns a process to produce a blank for optical fibers with thefollowing steps:

[0052] Guiding at least one liquid starting material through at leasttwo tubes having different diameters, wherein a first tube surrounds atleast a second tube,

[0053] Continuously uniting the starting material near the dischargeopening of the second tube in a diffusion zone and

[0054] Converting the material in the diffusion zone into the solidphase.

[0055] This process in accordance with the invention is suited inparticular for producing blanks for polycrystalline optical fibershaving several sections with different properties in the cross-sectionprofile. This is brought about by different liquid starting materialsbeing guided through different tubes during the production of a blank.The first tube corresponds in terms of its internal dimensions to theexternal dimensions of the blank being created. It can have a closedend. The second tube runs through the first tube and discharges into thefirst tube. Once the starting material has exited from the secondmaterial into the discharge area, the liquid starting materials of thefirst and second tubes are united. Then they are converted to the solidphase. In this way, a blank is created whose cross-section has a sectionwith dimensions corresponding approximately to the cross-section of thesecond tube. This section can be fabricated from a material, whichdiffers at least in terms of the index of refraction from the materialfed via the first tube.

[0056] The first and second liquid starting materials are directlyadjacent to one another near the discharge opening of the second tubeinto the first. A diffusion zone is formed. This is where a blending ofthe liquid starting materials takes places, predominantly or exclusivelyutilizing the diffusion. Control over the blending taking place is allthe better, the greater the share of diffusion is in the blending of thestarting materials.

[0057] The diffusion zone extends within the first tube in thelongitudinal direction from the discharge opening of the second tube upto a crystallization front, whose precise position is dependent upon thelocation where the temperature falls short of the melting temperature.This location can be preset as a process parameter.

[0058] The crystallization front is the boundary surface between theliquid and a solid phase. The shape of the boundary surface is afunction of the temperature distribution in the cross-sectional planesof the first tube. In addition, the shape of the boundary surface with amixture of two starting materials is a function of the concentration ofthe individual starting materials since the different starting materialshave different melting temperatures as a rule.

[0059] The degree of blending of the starting material fed via the firstand second tubes, for one, depends naturally on the materials used. Theinter-diffusion of two liquid starting materials is governed by thephysical properties of the two liquids.

[0060] The blending of the liquid starting materials can be influencedin a targeted manner, however, by process control, on the other hand.For example, the degree of blending of the different materials dependson the duration of blending. Diffusion will be stopped by quicklybringing about crystallization just after the liquid starting materialexits from the second tube. Relatively abrupt material boundaries arecreated along the cross-section in this manner. In the case of acylindrical fiber blank, stepped indices of refraction can be realizedin the radial direction in this way.

[0061] On the other hand, if diffusion is permitted over a longer periodof time by the materials in the diffusion zone being kept at atemperature above the melting point, a relatively extended diffusionzone is generated. In this way, a fiber blank can be realized with anindex of refraction profile in cross-section, which has one or even moresections of a gradual, continuous increase or decrease of the index ofrefraction. The gradient, i.e., the degree of the increase or decreaseof the index of refraction can be predetermined precisely with theprocess in accordance with the invention. The expansion of the diffusionzone in the cross-section plane shall be specified for this along withthe index of refraction of the starting material.

[0062] In order to realize a diffusion zone with a specific expansion ina cross-section profile, the wall thickness of the second tube can besuitable as a control parameter along with the diffusion duration. Acylindrical blank is considered as an example. The expansion of thediffusion zone in the radial direction can be influenced not just by thediffusion duration but also by the targeted selection of the thicknessof the wall of the second tube. A thicker wall increases the surface ofthe area in the cross-section profile of the fiber blank being generatedby the blending of the starting materials discharging from both tubes.However, it must be taken into account in this connection that withunfavorable conditions a non-homogenous blending can occur as a resultof uncontrolled flow conditions in the discharge area of the tubes.

[0063] The position of the diffusion zone in the cross-section profileof a fiber blank can be predetermined by a corresponding arrangement ofthe two tubes within the first tube.

[0064] Depending upon the desired cross-section profile of the fiberblank, for example with respect to its index of refraction, severaltubes can also be arranged within the first tube. Therefore, a secondand third tube can be used along with the external first tube for aW-shaped index of refraction profile of a cylindrical fiber blank. Thethird tube runs in through the second tube and the second one runsthrough the first tube. The tubes run concentrically. A first liquidstarting material is guided through the first and third tube and asecond liquid starting material is guided through the second tube. Inthe solid phase, the second starting material has a lower index ofrefraction than the first starting material.

[0065] The tubes do not have to be arranged concentrically, however. Thearrangement of the second, third, fourth, etc. tubes within the firsttube is determined in accordance with the desired cross-section profile.Fibers with three cores running next to one another, for example, canalso be produced in this way.

[0066] Of interest in this connection is an arrangement of differenttubes in a rectangular cross-sectional matrix in which the blank for anoptical fiber can be generated with several light channels separatedfrom one another whose arrangement corresponds to the arrangement ofsensors on a correspondingly detector so that the coupling between thedetector and optical fiber is especially simple.

[0067] In addition to the index of refraction of the fiber blanks, otherphysical parameter profiles can also be influenced in a targeted mannerwith the process in accordance with the invention, such as thetransmission profile, for example.

[0068] Of course, the process in accordance with the invention can alsobe used, however, for producing a blank that is homogenous in terms ofthe cross-section by the same material being guided through all tubes.It is also understood that blanks with the most varied externaldimensions and shapes can be produced with the process. In addition to acylindrical shape, blanks can also be produced in a cuboid shape. Onlycorrespondingly shaped tubes must be used. The first and second tubescan also have different cross-section shapes. For example, the firsttube can have the shape of hollow cube and the second tube can be ahollow cylindrical shape (at least in the area of its dischargeopening).

[0069] In connection with the already addressed optical fibers with amultiplicity of light channels, the types of light channelcross-sections that correspond in terms of shape with the shape of thesensors, i.e. that are square, are typical for optimal coupling of alight channel to a corresponding detector with a multiplicity of sensorsthat are arranged matrix-like. Even the outer cladding of the fibers canthen be square so that several fibers can be combined into a bundlewhereby the arrangement of all light channels in the bundle correspondsto the arrangement of the sensors on the detector.

[0070] The process in accordance with the invention is suitedparticularly for producing fiber blanks made of metal halides. It istypical that it be used to produce fiber blanks containing the materialsystem AgBr/AgCl in a solid solution. In this connection, areas withdifferent mixture ratios can be adjacent to one another. The mixingratio can change abruptly or gradually transverse to the longitudinalaxis of the fiber blank. Consequently, it is also possible to produceoptical fibers with index profiles in the infrared spectral rangebetween 4 and 18 micrometers with the process in accordance with theinvention. A fiber blank made of AgBr/AgCl produced with the process inaccordance with the invention has an especially homogenousmicrostructure.

[0071] In the case of an embodiment of the process in accordance withthe invention, until being united in the diffusion zone, the startingmaterials pass through a temperature profile in the longitudinaldirection of the tubes in such a way that the temperature of thestarting materials diminishes downstream and reaches approximately themelting temperature in the area of the discharge opening. The gradualcooling of the starting materials promotes the homogeneity of themicrostructure of the fiber blank being created.

[0072] In at least one embodiment of the inventive process, the firsttube is moved relative to the second tube in the direction of thediminishing temperatures in order to convert liquid starting material tothe solid phase.

[0073] The movement of the first tube relative to the second tube shouldtake place so that liquid starting material is always converted at aboutthe same distance from the discharge opening of the second tube into thefirst tube. This can be accomplished for example by the first tube beingmoved in the longitudinal direction in a furnace with a prescribedtemperature profile. The temperature profile is established so that themelting temperature is fallen short of at a prescribed distance from thedischarge opening of the second tube into the first tube and continuesto drop with increasing distance. Liquid starting material fed from thefirst and second tubes can flow into the diffusion zone due to themovement of the first tube relative to the second and subsequentlychanges to the solid phase when it has reached the prescribed distancefrom the discharge opening of the second tube. The transport ofcrystallized material away from the crystallization front is guaranteedin this way so that continuous growth of the blank is guaranteed. Due tothis process control, the length of the blank being produced is notlimited as a rule.

[0074] It is understood that instead of the movement of the first tube,the temperature profile and the second tube can also be shifted at thesame time in the longitudinal direction. As a result, the same relativemovement between the first tube and the second tube as well as thetemperature profile is realized. This alternative will no longer bementioned separately in the following for the sake of clarity of thedescription.

[0075] The speed of the relative movement from the first and second tubehas a substantial influence on the duration of diffusion at the boundarysurface between the first and second starting materials. Thecross-section profile of the optical properties of the blank beingproduced can be influenced by controlling the speed. If the liquidmaterial is moved into the diffusion zone at a relatively high speed inthe direction of the crystallization front, the diffusion time span isshort and the transition area between the first and second startingmaterials is of low expansion. This generates a cross-section profile ofthe index of refraction with a stepped progression. On the other hand,if the speed is low, the expansion of the transition area is larger andthe index of refraction profile has roughly linear and/or curvedsections.

[0076] Another possibility for influencing the forming cross-sectionprofile of the fiber blank is offered at this point: the progression ofthe index of refraction profile in the transition areas between thedifferent starting materials can also be influenced by the shape of thefront surface of the tube walls at the discharge opening. Essential inthis case are the position and shape of the front surface of the secondtube with respect to the position and shape of the crystallizationsurface. Because with constant speed of the movement of the first tube,the distance between the front surface of the tube and thecrystallization surface determines the duration of diffusion. If thisdistance varies in the radial direction over the extension of the wall,then the blending of the starting materials that are adjacent here isdependent upon the radial position. Basically curved or linear indexprogressions can be realized, as a result, by the corresponding shape ofthe front surface of the second tube in the transition area between thedifferent materials.

[0077] It is typical that a process be conducted with tubes whose frontsurface runs parallel to the crystallization surface. In this way, thediffusion duration is made independent of the radius. A linear indexprogression results in the transition area.

[0078] Blanks where the cross-section profile of an optical parameterchange in the longitudinal direction of the blank can be produced withthe process in accordance with the invention. In one embodiment, theindex of refraction profile is formed differently in the cross-sectionof a cylindrical blank in the longitudinal direction of the blank. Thisoccurs, for example, by changing the speed of travel of the first tube.As explained above, this changes the expansion of the transition areabetween adjacent materials. If the speed is increased approximately inthe course of producing a blank, the expansion of the transition area inthe cross-section decreases. In this way, a blank can be fabricatedwhich has an index of refraction that can be changed linearly in alongitudinal section and an index of refraction that can be changed in astepped manner in another longitudinal section.

[0079] Another inventive idea independently worthy of protectionconcerns a device to produce a fiber blank that includes at least twotubes, of which a first tube surrounds at least a second tube at leastin the area of one front surface of the second tube, and a heatingdevice, which is designed to generate a temperature profile in thetubes, which profile can be modified in the longitudinal direction ofthe first tube, whereby the cited front surface has a surface sectionwhose surface perpendicular forms an acute angle with the longitudinalaxis of the second tube.

[0080] The device in accordance with the invention is designed toexecute the process described above. In the case of this device, at itslongitudinal end where liquid starting material discharges into thefirst tube, the second tube has a front surface with a surface sectionwhose surface perpendicular forms an acute angle with the longitudinalaxis of the second tube.

[0081] To explain the invention it is assumed to begin with that, whenproducing fiber blanks, the phase boundary surface between the liquidstarting material and the solid blank is kept stationary by setting thetemperature profile correspondingly. This is easy to accomplish. Forexample, the first tube can be moved in a stationary temperature profilegenerated by the heating device. In this way, the fiber blank is allowto grow in the longitudinal direction by material being fed bit by bitthrough a zone of decreasing temperature. It always crystallizes theliquid starting material, which just passes the phase boundary surfacei.e., the location of the longitudinal expansion of the first tube atwhich the melting temperature is fallen short of. In the further courseof things, this material continues to cool.

[0082] With the formation of the front surface in accordance with theinvention a situation is achieved where, when operating the device, thediffusion zone described above has a longitudinal expansion for a fiberblank in the boundary area of different liquid starting materials thatvaries in the directions transverse to the longitudinal axis of thesecond tube. The longitudinal expansion of the diffusion zone is thedistance between the front surface of the second tube and the phaseboundary surface. As a result, the time span during which diffusion ispermitted between the adjacent starting materials is dependent upon theposition transverse to the longitudinal axis. This means, as describedwith the example of a cylindrical fiber blank, the diffusion time spanis dependent upon the radial distance from the longitudinal axis to thesecond tube. The blending of the neighboring starting materials variesautomatically with the diffusion time span, however. And the opticalproperties, for example, vary in turn with blending. In this connection,reference is made to the solid solution of AgBr/AgCl already mentionedabove.

[0083] Consequently, a fiber tube can be produced with the device inaccordance with the invention, which has gradual, linear or non-lineartransitions of the index of refraction profile. The type of respectivetransition can be influenced by the design of the front surface.

[0084] A stationary phase boundary was assumed with the previousrepresentation. In the case of the device in accordance with theinvention, the diffusion duration is itself then a function of theradial distance, however, if the phase boundary surface between liquidand crystal in the longitudinal direction of the first tube is moveableand not stationary. However, in this case control over the change of themixing ratio in the diffusion zone is more expensive to realize sincethe movement of the phase boundary must also be taken intoconsideration.

[0085] The most varied designs of the front surface of the second tubeare advantageous. Because, as a rule, the special formation of the frontsurface depends upon the desired cross-section profile of the index ofrefraction. Common to all formations is that there is a front surfacesection whose surface perpendicular forms an acute angle with thelongitudinal axis of the second tube. This surface section can be flator curved.

[0086] In one embodiment of the device of the invention, the frontsurface of the two tubes runs parallel to a phase boundary surfacebetween a liquid and a solid phase of the starting material that formsduring device operation at a distance before the tube discharge opening.In the case of this embodiment, the diffusion time span is consequentlyconstant in the radial direction. Therefore, a particularly exactlypredictable index of refraction profile can be formed which runs steeperor flatter depending upon the diffusion duration.

[0087] In this connection, the front surface in one embodiment isdesigned to be curved. A curved phase boundary surface occurs, forexample, with the creation of a solid solution of AgCl/AbBr with achlorine concentration from the molten mass that varies in the radialdirection. The melting temperature of this solution is approximatelylinearly dependent upon the concentration of the chlorine in thesolution. As a result, areas of low chlorine concentration have a lowermelting point than areas of higher chlorine concentration. As a resultof diffusion, an area with a variable melting temperature in theradiation direction is created in the diffusion zone between areas withdifferent chlorine concentrations. The varying melting temperatureallows a phase boundary surface to be created between liquid and solidsilver halides, which follows the prevailing temperature profile in theradial direction of the chlorine concentration, for one, and, on theother hand, in the longitudinal direction of the first tube.

[0088] In another embodiment, the front surface is curved convexly. Aconvex curvature correspond to the shape of the phase boundary surfaceforming in the first tube, if the material in the core of the fiberblank being produced has a lower melting temperature than in the area ofthe cladding. Consequently, a concave curvature of the front surface isused with opposite conditions.

[0089] The first tube is mounted so that it is displaceablelongitudinally in one embodiment. The advantages of this embodiment wereexplained in detail above on the basis of the description of theprocess.

[0090] A further aspect of the invention that is independently worthy ofprotection is a process to produce an optical fiber from a blank made ofraw material, in which the blank raw material is extruded through anozzle. The nozzle is set in vibration in the case of the process inaccordance with the invention.

[0091] In the extrusion of raw material, raw material particles in thesize of several micrometers are pressed through a nozzle and therebyconnected. A micro-crystallite structure is generated in this process.The process in accordance with the invention solves the problem that,when pressing the crystallite of the blank through the nozzle, largergas-filled interstices can form between neighboring micro-crystallitesin the fibers being generated. This problem is avoided with the processin accordance with the invention by the nozzle being set in vibration. Aperiodic pressure increase and decrease is superimposed on the extrusionpressure exerted on the material by the nozzle. As a result, thecrystallites that are in contact with the nozzle are set in vibration.These interact with other crystallites due to the vibration. Thisvibration shakes the crystallites in such a way that the gas intersticesbetween them are minimized. The crystallites are pressed more compactlythan with known processes. As a result, the leakage of gas filledinterstices at the boundary surface and the micro-crystallites arestrongly reduced.

[0092] The nozzle is set in ultrasonic vibration in at least oneembodiment of the invention.

[0093] The vibration is transmitted to the nozzle via a ram in a furtherembodiment of the invention.

[0094] An extrusion device that is independently worthy of protection,which is designed to execute the process in accordance with theinvention, is comprised of a ram that can be displaced longitudinallyand a nozzle. In accordance with the invention, the nozzle is coupledwith means to generate vibrations. The means to generate vibrations cancontain a piezoelectric crystal.

[0095] In the case of this embodiment, the blank is located in a chamberinto which the ram is pressed. Alternatively, it is also possible tokeep the ram stationary with the nozzle and move towards the nozzle andthe ram with the blank in the chamber. Particularly in this case thechamber can also be set in vibration. A piezoelectric vibrationmechanism, which acts either on the chamber or, as already described, onthe ram is used for this, for example.

[0096] A further aspect of the invention that is independently worthy ofprotection concerns an extrusion device, whose nozzle has an exitsection whose shape deviates from the external cross-section of theblank so that fibers with a square or other cross-section can beextruded starting with round blanks, for example.

[0097] A further aspect of the invention that is independently worthy ofprotection concerns an optical fiber with a fiber end where areflection-reducing microstructure is provided on the end of the fiber.

[0098] The optical fiber in accordance with invention has the advantagethat a reflection-reducing microstructure directly on the end of thefiber at the same time forms protection for the inside of the fiber. Asa result, the fiber is less sensitive to environmental influences.

[0099] The microstructure is impressed on the fiber material with oneembodiment of the invention.

[0100] Alternatively, an element affixed to the end of the fiber thathas the microstructure can be provided. The element is usually resistantto chemical substances that are present in its environment. The elementis fabricated of artificial diamond in one embodiment.

[0101] As a supplement to the microstructure for example, the elementcan contain a radiation filter that is permeable for certain wavelengthsor be used alone as a radiation filter.

[0102] In another embodiment an optical fiber is provided with amicrostructure that is designed in such a way that at least a portion ofthe radiation emerging from the end of the fiber is scattered.

[0103] Another inventive idea independently worthy of protectionconcerns an optical fiber, which comprises several light channels. Theselight channels are primarily formed by cylindrical cores with a firstindex of refraction inside the fiber, which are enclosed by a claddingwith a second index of refraction and are separated from one another bythe cladding. Electromagnetic radiation with suitable wavelengths isfully reflected in the boundary area between the cladding and therespective core. The advantage of this type of fiber for one is that,due to the great number of light channels, a greater quantity ofinformation can be transmitted through the fiber than is the case withconventional optical fiber with a single light channel. In addition, itis possible to use these fibers to conduct spectral analyses onexamination objects. To do this, wideband electromagnetic radiation isguided through a first core to the examination object. A simplelight-emitting diode can be used as a source of radiation. The lightreflected on the examination object is then guided back through a secondcore of the fiber. Conclusions about the condition of the examinationobject can then be drawn from the spectrum of reflected light. As aresult, spectral analyses can be conducted on poorly accessibleexamination objects.

[0104] An advantageous development of the fiber with several cores isattaching spectral filters on at least one of the ends of the fiber.These spectral filters are usually attached on at least one end of thecores. The spectral filter has the property of only being permeable forradiation with specific wavelengths. Consequently, the radiation exitingfrom the end of the light channel with the spectral filter only haswavelengths that match the spectral filter.

[0105] Various devices can be used to decouple and transmit theelectromagnetic radiation from the cores to detectors. For one, it ispossible to project the end of the fiber by means of lenses on a plane.The image of the end of the fiber on the plane should represent anenlargement. A detector can pick up the radiation exiting from the coreby the detector being placed in the area of the projection plane wherethe end of the light channel is reproduced. Thus, the radiation exitingfrom one of the cores can always be fed separately to the detector.Since the image of the end of fiber in enlarged on the projection plane,the distances between the light channels on the projection plane arealso greater so that it is simpler to detect the radiation exiting fromthe light channels separate from one another.

[0106] With respect to coupling a fiber to a detector, in particular anoptical fiber with several light channels that are separated from oneanother, it is especially simple to create a fiber whose arrangementcorresponds to the arrangement of the sensors on the correspondingdetector, so as to couple the detector with the optical fiber. One sucharrangement of a plurality of light channels in an optical fiber is amatrix with a rectangular cross-section.

[0107] In the case of optical fibers with a plurality of light channels,such light channel cross-sections, whose shape corresponds to the shapeof the sensors, i.e., are square, are used for optimal coupling of alight channel to a corresponding detector with a multiplicity of sensorsthat are arranged in a matrix-like manner. Then the external cladding ofthe fiber can also be square so that several fibers can be combined intoa bundle, whereby the arrangement of all light channels in a bundlecorresponds to the arrangement of the sensor on the detector.

[0108] In addition, it is possible to use a bifurcated fiber in order todecouple the radiation exiting from the light channels separately fromone another. The bifurcated fiber has three ends. The first end, atwhich a first and a second light channel end, a second end, at which thefirst light channels ends, and a third end, at which the second endends. The two light channels branch at the bifurcation in order to runthrough the branches of the bifurcation separate from one another.

[0109] Producing a bifurcated fiber can be accomplished, for example, bytwo fibers being laterally beveled up to the area of a core so thatlight can exit from the channel. The beveled areas are then attached toone another in such a way that light can penetrate via the groundsurfaces from one core of a fiber into the adjacent core of the otherfiber.

[0110] Another independent inventive idea concerns an optical fiber witha core in which an optically active material is located. The opticallyactive material is characterized in that it can be excited by the lightpassing through the core, i.e., the optically active material absorbsthe light, after which it adopts a higher energy state. This type offiber is suitable for producing a laser. The optically active materialin the fiber is excited by optical pumping, i.e., by coupling insuitable light or electromagnetic radiation in such a way that apopulation inversion occurs. The number of excited states exceeds onaverage over time the number of non-excited states. The laser light isgenerated by stimulated emission of radiation and exits from the end ofthe light channel. In order to make a resonator available for the laserlight, the ends of the optical fiber are commonly mirrored with one ofthe mirrors being partially permeable for the laser light so that it canexit from the fiber.

BRIEF DESCRIPTION OF THE DRAWINGS

[0111] The invention will be understood best when reference is made tothe accompnaying drawings, wherein identical part numbers identifyidentical parts, and wherein:

[0112]FIG. 1 is a very simplified sectional representation of a reactorto produce and purify liquid starting material as well as to produce afiber blank;

[0113]FIG. 2a is a perspective principle diagram of a device to producea fiber blank;

[0114]FIG. 2b is a sectional view of the device from FIG. 2a;

[0115]FIG. 2c is a sectional view of another device to produce a fiberblank;

[0116]FIG. 2d is a sectional view of another device to produce a fiberblank;

[0117]FIG. 3 is a schematic, very simplified sectional view of anotherdevice to produce a fiber blank;

[0118]FIG. 4a is a sectional view of the device of FIG. 3;

[0119]FIG. 4b is a diagram that shows different dependencies of theindex of refraction from the radial position with three differentcylindrical fiber blanks that were produced by the device in accordancewith FIG. 4a;

[0120]FIG. 5a is a schematic, very simplified sectional view of anotherdevice to produce a fiber blank;

[0121]FIG. 5b is a diagram that shows the dependence of the index ofrefraction from the radial position with another cylindrical fiber blankthat was produced by the device in accordance with FIG. 5a;

[0122]FIG. 6a is a simplified representation of an extrusion device toproduce an optical fiber;

[0123]FIG. 6b is a simplified representation of another extrusion deviceto produce an optical fiber;

[0124]FIG. 7a is a profile of the end of a fiber of an embodiment of anoptical fiber in accordance with the invention;

[0125]FIG. 7b is a perspective view of the end of the fiber inaccordance with FIG. 7a;

[0126]FIG. 8a is a cross-section of a fiber with several cores;

[0127]FIG. 8b is a cross-section of another fiber with several cores;

[0128]FIG. 8c is an optical fiber with light channels of a squarediameter arranged in accordance with a square matrix;

[0129]FIG. 8d is an optical fiber with a square external cross-section;

[0130]FIG. 9 is a fiber bundle made of several fibers in accordance withFIG. 8d;

[0131]FIG. 10 is a schematic view of a device to project a fiber end ona projection plane;

[0132]FIG. 11 is a side view of a bifurcated fiber; and

[0133]FIG. 12 is an optical fiber with a light channel with arectangular cross-section.

DETAILED DESCRIPTION OF THE DRAWINGS

[0134]FIG. 1 shows in a very simplified sectional representation areactor 10 to produce and purify liquid starting material as well as toproduce a fiber blank. The reactor 10 forms a cylindrical reactorchamber 12 whose walls 14 are provided with a heating device 16. Justthe heating spirals 18 of the heating device are shown in FIG. 1.

[0135] A cylindrical container 20, which surrounds a tube 22, isarranged in the reactor chamber 12. The tube 22 can be connected viaconnectors that are not shown with external vacuum pumps and with gascontainers to produce a vacuum or an inert gas atmosphere. A container24 is attached within the tube 22. The container 24 is designed toaccommodate liquid metal. In addition, the container 24 is connected viagas tubes 26 and 28 with two externally attached halogen gas sources 30and 32. The liquid starting material for producing the fiber blank isextracted from the liquid metal and the gases originating from thehalogen gas sources 30 and 32. The composition of the liquid startingmaterial is determined by the respective partial pressure of the halogengases above the liquid as well as by the temperature in the container24. So that the starting material is free of impurities, the containeris evacuated before the halogen gases are introduced. As a result, thenumber of undesired reactive atoms or molecules in the container is verymuch reduced. In addition, an inert gas, i.e., a reaction-resistant gassuch as nitrogen gas or a noble gas is introduced into the container 24.This gas prevents any undesired reactive gases that might be remainingin the container from reacting with the liquid. It is typical that aninert gas be selected that is heavier than the conceivable undesiredreactive gases such as oxygen gas or water vapor or their gaseousreaction products so that the undesired reactive gases do not contactthe liquid. Not shown are means to set the partial pressure of the twohalogen gases in container 24. The halogen gases entering from thesources 30 and 32 are brought to a reaction with the liquid metal in thecontainer 24. For example, liquid silver and the halogen gases bromineand chlorine are brought to a reaction here so that liquid mixture ofAgBr and AbCl is created. The container can be heated to a suitablereaction temperature for this purpose.

[0136] The container 24 is cylindrical to a large extent, but tapers,however, towards the bottom like a funnel and discharges at the outsidewall of a hollow cylindrical tube 34. The tube 34 runs concentricallywithin the container 24 and extends over the largest portion of itslongitudinal extension. The wall of the tube 34 is porous as far as thetube extends within the container so that liquid AgBr and AgCl canpenetrate from the container into the tube and flow through the tubetowards the bottom and out. The liquid starting material passes througha filter 36 before the exit from the tube 34.

[0137] Following the container 24 downward are a number of capillarypurification stages, of which two purification stages 38 and 40 areshown here. The purification stages 38 and 40 are funnel-shaped andcontain a capillary filter material. The liquid starting material runsthrough these purification stages and collects after exiting from thelast purification stage 40 in a starting material bath 42 in the lowerarea of tube 22. The starting material bath 42 is positioned on a solidblank section 44, which is generated towards the bottom from the liquidstarting material bit by bit by cooling under the melting temperaturewith constant feed of the tube 22.

[0138] The tube 22 along is attached in a displaceable manner togetherwith the container 20 along the reactor chamber. The storage, drive andcontrol devices provided for this purpose are not shown in FIG. 1 forthe sake of simplicity.

[0139] The heating device 16 is designed in such a way that temperatureprofile that can be modified in the longitudinal direction of thereactor chamber 12 can be set. An example of this type of temperatureprofile is shown in FIG. 1 to the right of the reactor 10 in the form ofa temperature diagram 46. In the temperature diagram 46, an abscissa 48runs from the top to the bottom deviating from the normalrepresentation. Marked on the abscissa 48 are positions x along thelongitudinal extension of the reaction chamber 12 depicted to the leftof the diagram relative to the upper edge of the reactor chamber.Temperature T in the reactor chamber 12 is marked on the ordinate 50,with the temperature values on ordinate 50 in temperature diagram 46increasing from the left to the right. The temperature profile shownhere is therefore the dependence of the temperature T in the reactorchamber 12 from position x along the longitudinal direction of thereactor chamber.

[0140] Temperature value T_(s) is identified on ordinate 50 andindicates the melting temperature of the liquid starting material. Thisvalue is also marked in diagram 46 by a dashed line running parallel toabscissa 48.

[0141] A temperature curve 52 indicates the progression of thetemperature in the reactor chamber 12. In the upper area of the reactorchamber, the temperature is above the melting point and dropscontinuously towards the bottom until it reaches the melting temperatureat a point indicated with x_(k). This point is identified with a cross54 in diagram 46.

[0142] A dashed line 56 indicates that the boundary between the startingmaterial 42 and the solid section 44 of the fiber blank lies at thislevel in tube 22. By gradually guiding the tube 22 downward morestarting material is continuously cooled below the melting point andcrystallized.

[0143]FIG. 2a shows a perspective principle diagram of a device toproduce a fiber blank. FIG. 2b shows a cross-sectional view of the samedevice. The device contains a vessel 60, which has approximately theshape of a hollow cylinder cut through in a center plane. The vessel 60accommodates a starting material bath 62, which is composed for exampleof a liquid AgCl/AgBr mixture. A solid, cylindrical core 64 is partiallysubmerged in the starting material bath 62. The core 64 is positioned ina storage device 66 (only indicated here in principle) so that it can berotated around its longitudinal axis 68. The storage device 66 isdesigned in such a way that the core can be shifted upwards or downwardsrelative to the bath.

[0144] When rotating the section of the core 64 submerged in thestarting material bath 62, liquid starting material adheres to itsurface. After this section emerges from the bath 62, the adheringliquid starting material cools and crystallizes. When it is re-submergedin the bath, this material forms the surface for the adhering ofadditional liquid starting material. The cylindrical core 64 grows bitby bit in the radial direction in this way.

[0145]FIG. 2c shows another device to produce a fiber blank. To a largeextent, the device is identical to the device shown in FIGS. 2a and 2 b.In addition, the device in FIG. 2c includes a heating device 63 to setthe temperature of the bath 62. The heating device sheaths the vessel 60to a large extent so that the temperature of the liquid can be setprecisely. Further, the device in FIG. 2c is planned to create a fiberblank whose index of refraction changes radially continuously. To dothis, the composition of the starting material is modified in the courseof the core's 64 growth. Funnels 61 containing a starting material withanother mixing ratio of AgBr and AgCl than in the bath are provided forthis purpose. The liquid from the funnels is mixed with the bath 62 inthe course of the growth of the fiber blank. The index of refraction ofthe fiber blank is supposed to be unchangeable in the direction of itslongitudinal axis. As a result, one must always make sure that theliquid starting material in the bath is a homogenous mixture. Attachedto the underside of the vessel is a vibration device, which shakes thecontainer 60 in such a way that the liquid originating from the funnels61 is distributed homogenously in the bath 62. The frequency andamplitude of the vibration must be adjusted suitably for optimalblending of the liquid. The vibration device includes severalpiezoelectric crystals that are attached along the container and aretriggered simultaneously by an alternating voltage source.

[0146]FIG. 2d shows a sectional view of another device to produce afiber blank. To a large extent, this device corresponds to the one shownin FIG. 2c. Instead of a vibration device, the device includes tubulargas lines 67 to transmit inert gases through the liquid. The gas lines67 are located on the floor of bath 62 and extend over the entire lengthof the bath 62. Located on the upper side of the gas lines 67 areopenings (not shown) from which the gas exits and rises vesicularly tothe surface of the liquid. Nitrogen or a noble gas is commonly used asthe inert gas. The gas bubbles flowing through the liquid provide forblending of the liquid. The gas lines 67 are arranged in such a way thatthe gas bubbles rise between the core 64 and the liquid mixed in via thefunnel in order to guarantee optimal blending.

[0147]FIG. 3 shows a section of another device to produce a fiber blank.The device is fundamentally similar to the device 10 described on thebasis of FIG. 1. The reactor chamber is not described in further detailin this case. The present device has a first tube 70 within the reactorchamber. A second tube 72 with a smaller diameter projects into thefirst tube 70. The first tube 70 can be displaced in the direction ofits longitudinal axis against the second tube 72.

[0148] In the case of the present device, producing a fiber blank takesplace basically as described on the basis of FIG. 1, namely by cooling astarting material 74. For this purpose the tube 72 is shiftedcontinuously downwards along a temperature profile 75.

[0149] In contrast to the device in accordance with FIG. 1, the startingmaterial 74 in this case is composed of different components, however.While a first liquid starting material is fed through the external,first tube 70, a second starting material is fed through the internal,second tube 72. In the case of the first starting material, one isdealing with the starting material for the cladding of an optical fiber,in the case of the second starting material with the starting materialfor the core of the optical fiber. The material for the core [is]AgCl/AgBr with a ratio of 3 to 1 for example.

[0150] Consequently, the first and second tubes with different feedssystems for liquid starting material are connected, which is indicatedin FIG. 3 by three different purification stages 76 and 80. Thepurification stages 76 discharge into the first tube 70 and thepurification stage 80 discharged into the second tube 72.

[0151] The different starting materials come into contact with oneanother in the area of the discharge opening of the second tube 72 intothe first tube 70. A cylindrical diffusion zone 84 forms between thesecond tube 72 and a crystallization surface 82 under the wall of thesecond tube 72. A blending of the different starting materials based onflows can be prevented by correspondingly slow process control. In thecase of silver halides, these types of flow problems basically do notplay an essential role, however.

[0152] The front surface 86 of the second tube 72 is formed parallel tothe phase boundary surface. In this way, it is guaranteed that theduration of the diffusion is independent of the radial position.

[0153] The shape of the crystallization surface 82 depends upon themelting temperatures of the starting materials used and the temperatureprofile 75. In the present case, the first starting material fed throughthe first tube 70 has a higher melting temperature T_(S1) than thesecond starting material fed through the second tube 72, which has amelting temperature of

[0154] The temperatures T_(S1) and T_(S2) are reached in the reactorchamber at different positions x₁ and x₂. As a result, thecrystallization surface extends in the longitudinal direction of thefirst tube 70 between these positions x₁ and x₂. In the radial directionof the tube 70, the position of the boundary surface between the liquidand the solid phase is dependent upon the mixing ratio between the twostarting materials. The larger the portion of the first startingmaterial, the closer the phase boundary surface lies to position x₁. Thelarger the portion of the second starting material, the closer the phaseboundary surface lies to position x₂. In the present case, a convexlycurved phase boundary surface 82 forms between the two startingmaterials as a result of the diffusion.

[0155] With given starting materials and a given temperature profile inthe reactor chamber, the precise shape of the phase boundary surface 82can be calculated on the basis of the melting temperature of the purestarting material and its mixtures.

[0156] The solid fiber blank with a core 88 composed of the crystallizedsecond starting material forms beneath the phase boundary surface.Externally the blank has a cladding made of the first starting material.A transition area 92 is located between the core 88 and the cladding 90.

[0157]FIG. 4a shows the device to produce a fiber blank in accordancewith FIG. 3. Next to it, FIG. 4b shows a diagram that shows thedependence of the corresponding index of refraction on the radialposition in the case of three different cylindrical fiber blanks. Adifferent line type is assigned to the index of refraction of each fiberblank. A solid solution of AgBr/AgCl with different mixing ratios in thecore and cladding is always shown as an example. The pure claddingmaterial has an index of refraction of 2.1 and the pure core materialhas an index of refraction of 2.2. Only the diffusion duration beforeconversion of the starting material bath into the solid phase wasvaried.

[0158] The solid line 94 is an index of refraction profile with arelatively sharp, almost step-shaped transition almost without atransition area. It corresponds to a short diffusion duration. Thedashed line 96 shows, on the other hand, a slightly rounded index ofrefraction profile corresponding to an average diffusion duration. Atransition area with indices of refraction that gradually drop from 2.2to 2.1. is located between the core and cladding. Finally, the dashedand dotted line 98 shows a very rounded index of refraction profile witha transition area of great expansion. This is the result of anespecially long diffusion duration before crystallization.

[0159]FIG. 5b shows a diagram with the dependence of the index ofrefraction on the radial position with another cylindrical fiber blank.Next to it, FIG. 5a shows another device to produce a fiber blank. Thisdevice represents a modified embodiment of the device in accordance withFIG. 3. In this device, the second tube 72 runs within a third tube 73.The first tube 70 in turn surrounds the third tube. The startingmaterial fed through the second tube 72 corresponds to the startingmaterial fed through the first tube and has an index of refraction of2.2 in a solid phase, for example. Now a starting material that has anindex of refraction of 2.1 in a solid phase, for example, is fed throughthe third tube 73. A fiber blank with a W-shaped index of refractionprofile 100, which is shown in the diagram in FIG. 5b, is generated as aresult of the diffusion. In addition, an annular piezoelectric elementarrangement 75 and 77, which is triggered by means of an alternatingvoltage generator (not shown), is attached to the tube 72 and 73. Thetubes 72 and 73 are thus set into a vibration along their longitudinalaxis that is predetermined by the alternating voltage generator. Thiscauses a greater blending of the starting materials in the diffusionzones beneath the tubes 72 and 73. Therefore, the progression of theindex of refraction can be set. Greater blending causes a less steepprogression of the index of refraction in the area of the diffusionzone. A lesser blending has the opposite effect.

[0160] These types of W-shaped gradient index of refraction profileshave the advantage that the core-cladding structure of a fiber isgenerated at the same time as the crystal pulling process and not duringthe subsequent extrusion process. Especially low concentrations ofimpurities are achieved in this way, which in the conventionalproduction process concentrate just at the boundary surface of the coreand cladding.

[0161]FIG. 6a shows a simplified representation of an extrusion device102 to produce an optical fiber 104. The extrusion device 102 has anapproximately cylindrical high-pressure chamber, which is enclosed byheat-conducting walls 106. A heating device 108 surrounds the walls.

[0162] A longitudinally displaceable ram 110 engages in thehigh-pressure chamber. The ram 110 has a centric bore hole 112 extendingover the entire length. The ram 110 is in contact at its longitudinalend with a nozzle 14 in the high-pressure chamber. On the oppositelongitudinal end, the ram 110 is provided with a vibration device 116having piezoelectric element, which is connected to a power supply andfrequency generator unit 118.

[0163] The nozzle 114 has a nozzle opening that is concentric with thebore hole 112. Its side facing the reactor chamber has a surface curvedtowards the nozzle opening. This surface is in contact with a fiberblank 120.

[0164] To produce an optical fiber, the ram exerts a force of pressureon the fiber blank 120 via the nozzle. At the same time the vibrationdevice generates a vibrational force superimposed on the force ofpressure of the ram 110, which is transmitted via the ram and nozzle 114to the fiber blank 120. As a result, a periodic increase and decrease inpressure is superimposed on the extrusion pressure exerted by the nozzle114 on the fiber blank 120. The crystallites of the fiber blank that arein contact with the nozzle 114 are thereby set in vibration. Theseinteract due to the vibration with other crystallites of the fiberblank. This vibration shakes the crystallites in such a way that the gasinterstices between them are minimized. This provides for an especiallydense distribution of the micro-crystallites in the optical fiber 122projecting downward in the bore hole 112 of the ram 110 of the extrusiondevice 102.

[0165]FIG. 6b shows a simplified representation of an extrusion device102, which differs from the extrusion device shown in FIG. 6a in thefollowing details. The ram 110 of the extrusion device is designed torest on a base 111. The base 111 has an opening through which theoptical fiber 104 is extruded. The high-pressure chamber 120 is pressedon the ram 110 in order to extrude the fiber 104 from the opening of thebase 111. The piezoelectric elements of the vibration device 116, whichare connected to a power supply and frequency generator unit 118, areprovided in area of the wall 106 that is opposite from the ram 110. Thisarrangement of the vibration device has the advantage that thepiezoelectric element does not have to bear the weight load of thechamber 120 and the wall 106 bordering it and the heating device 108.

[0166]FIG. 7a shows a profile of an optical fiber 126 fabricated ofmetal halides in the area of a longitudinal end. FIG. 7b shows aperspective view of the same area. The sectional plane of therepresentation in FIG. 7a runs in a center plane containing thelongitudinal axis of the cylindrical fiber 126.

[0167] The fiber 126 has a reflection-reducing microstructure 130 on afront surface 128. The microstructure is composed here of approximatelycuboid elements arranged periodically in two directions that aremutually perpendicular, an x-direction and a y-direction. The periods,that is the distance between the same sections of neighboring elementsis designated with L in FIG. 7a and is identical here in the x-directionand the y-direction. The period L is a function of the wavelength rangein which the fibers are supposed to operate. The period is approximately2 micrometers for wavelengths between approx. 8 and 12 micrometers. Therepresentations in FIGS. 7a and 7 b do not reproduce these dimensions toscale.

[0168] The side length of the cuboids is designated with a. Bystipulating the relationship L/a, the so-called filling factor, theeffective index of refraction of the microstructure can be set to avalue between that the of fiber and that of the surrounding medium, airfor example. To produce a Lambda/4 layer, the effective index ofrefraction is selected as the geometric mean of the two indices ofrefraction for fiber and air. Utilizing diffraction effects, areflection-reducing surface of the fiber is thereby generated.

[0169]FIG. 8a shows a cross-section of a fiber with several channels orcores 142. The channels 142 are formed cylindrically and pass throughthe optical fiber along its entire longitudinal extension. Threechannels 142 are shown in FIG. 8a, which are separated from one another.The cladding 140 is located between the channels 142. The cladding iscomposed of a material having another index of refraction than the indexof refraction in the cores. Due to the difference between the indices ofrefraction, there is a full reflection of light at the boundary surfacebetween the fiber-optic light guides and the cladding. The lightradiation located in the channels cannot leave them and is guidedthrough the fiber. Since the channels are separated from one another bythe cladding 140, the light directed through a channel cannot get intoone of the adjacent channels.

[0170]FIG. 8b shows a cross-section of another optical fiber withseveral channels or cores 146. In contrast to the fibers in FIG. 8a, thecores do not have a circular cross-section profile, rather they formsegments of a circle of various sizes. The channels are formed by acladding 144 forming a border that is essentially circular incross-section, which is infiltrated by a T-shaped section of thecladding 144.

[0171]FIG. 10 shows a schematic side view of a device to project the endof a fiber on a projection plane 154. An optical system 152 that makessure that the end of the fiber is depicted in focus on the projectionplane 154 is arranged between the end of the fiber 150 and theprojection plane 154. The optical system 152 is made up of one or morelenses whose focal depth and distances from one another and to the endof the fiber 150 and the projection plane 154 are selected in such a waythat an in-focus and enlarged image appears on the projection plane 154.

[0172]FIG. 11 shows a side sectional view of a bifurcated fiber. Thebifurcated fiber includes two cores 160, 162 that are surrounded by acladding 164, which serves to separate them. Initially, the cores 160,162 run parallel to one another through the fiber up to the bifurcation.There they run separate from one another each through one of the twofiber strands or branches 166 that continue on from the bifurcation.

[0173] Numerous variations of the devices and process presented arepossible within the framework of the respective inventive idea. Thefibers produced are usually formed from polycrystalline infrared fibers.For example, the chemical reaction between halogen gases and liquidmetal to form metal halides can also be brought about in a reactive gasatmosphere. In the case of the extrusion device, the vibrational forcecan also be exerted directly on the nozzle or directly on the fiberblank. The optical microstructure on the end of the fiber can also bedesigned to focus the exiting or entering light, or to refract, or todeflect, or for an increased reflection.

[0174] Produced infrared fibers are subsequently introduced into apolymer tube with high rigidity, high temperature resistance, lowpenetrability for oxygen, moisture and other environmental substancesand hermetically sealed. The polymer material can be apoly-etherether-ketone (PEEK) or a fluorinated polymer such as TEFLON.

What is claimed is:
 1. A process for manufacturing a starting materialfor an optical fiber, the starting material containing metal hialidesand having a predetermined refractive index, the process comprising thesteps of: mixing halogen-containing gases to form a gas mixture with apartial pressure ratio, upon which the predetermined refractive indexdepends; causing the gas mixture to react chemically at a firsttemperature with a metal to form a reaction product having a meltingpoint, such that the first temperture is at least the melting point; andcooling the reaction product to a second temperture below the meltingpoint.
 2. The process of claim 1, wherein the reaction product is asolid solution of metal halides.
 3. The process of claim 1, wherein themetal is selected from a group consisting of the alkali metals, thalliumand silver.
 4. The process of claim 2, wherein the metal is selectedfrom a group consisting of the alkali metals, thallium and silver. 5.The process of claim 4, wherein the solid solution contains silverbromide, silver chloride or a combination of silver bromide and silverchloride.
 6. The process of claim 3, wherein the solid solution containssilver bromide, silver chloride or a combination of silver bromide andsilver chloride.
 7. The process of claim 5, wherein thehalogen-containing gas contains bromine.
 8. The process of claim 6,wherein the halogen-containing gas contains bromine.
 9. The process ofclaim 1, wherein the halogen-containing gas contains bromine.
 10. Theprocess of claim 7, wherein the halogen-containing gas containschlorine.
 11. The process of claim 8, wherein the halogen-containing gascontains chlorine.
 12. The process of claim 9, wherein thehalogen-containing gas contains chlorine.
 13. The process of claim 1,wherein the halogen-containing gas contains chlorine.
 14. The process ofclaim 10, wherein the gas mixture partial pressure ratio is set so thatthe solid solution contains bromine and chlorine in a particle numberratio of 3 to
 1. 15. The process of claim 14, further comprising thestep of: purifying the reaction product before the cooling step belowthe melting point thereof.
 16. The process of claim 11, furthercomprising the step of: purifying the reaction product before thecooling step below the melting point thereof.
 17. The process of claim12, further comprising the step of: purifying the reaction productbefore the cooling step below the melting point thereof.
 18. The processof claim 13, further comprising the step of: purifying the reactionproduct before the cooling step below the melting point thereof.
 19. Theprocess of claim 15, wherein the cooling step is achieved while feedingthe reaction product in a furnace along a temperature gradient in afurnace from the first temperature to the second temperature.
 20. Theprocess of claim 16, wherein the cooling step is achieved while feedingthe reaction product in a furnace along a temperature gradient in afurnace from the first temperature to the second temperature.
 21. Theprocess of claim 17, wherein the cooling step is achieved while feedingthe reaction product in a furnace along a temperature gradient in afurnace from the first temperature to the second temperature.
 22. Theprocess of claim 18, wherein the cooling step is achieved while feedingthe reaction product in a furnace along a temperature gradient in afurnace from the first temperature to the second temperature.
 23. Aprocess for manufacturing a blank for optical fibers, comprising thesteps of: guiding at least one molten starting material through at leasttwo tubes having different diameters, wherein a first of the at leasttwo tubes surrounds a second of the at least two tubes; continuallybringing together the staring material near a discharge opening of theseond tube in a diffusion zone; and converting the starting materialthrough the diffusion zone in a solid phase.
 24. The process of claim23, wherein the guiding step comprises: guiding at least two moltenstarting materials which differ in the concentration of the constituentsthereof.
 25. The process of claim 24, wherein the starting materialspass through a profile of diminishing temperature in the longitudinaldirection of the tubes until being united in the diffusion zone, so thatthe temperature of the starting materials reaches the meltingtemperature thereof in the area of the discharge opening.
 26. Theprocess of claim 23, wherein the starting materials pass through aprofile of diminishing temperature in the longitudinal direction of thetubes until being united in the diffusion zone, so that the temperatureof the starting materials reaches the melting temperature thereof in thearea of the discharge opening.
 27. The process of claim 25, wherein thefirst tube is moved relative to the second tube so that the moltenstarting material is always converted at about the same distance fromthe discharge opening of the second tube into the first tube.
 28. Theprocess of claim 26, wherein the first tube is moved relative to thesecond tube so that the molten starting material is always converted atabout the same distance from the discharge opening of the second tubeinto the first tube.
 29. An apparatus for a process for manufacturing ablank for optical fibers, comprising: at least two tubes; a first of theat least two tubes surrounding a second tube of the at least two tubesin at least a front surface of the second tube, and a heating apparatusfor producing a temperature profile in the at least two tubes, theprofile changeable in a longitudinal direction of the first tube,wherein the front surface has a surface section, a perpendicular theretoforming an acute angle with a longitudinal axis of the second tube. 30.The apparatus of claim 29, wherein the front surface runs parallel to aphase boundary surface between a liquid and a solid phase that forms ata distance before the tube discharge opening while operating theapparatus.
 31. The apparatus of claim 30, wherein the front surface iscurved.
 32. The apparatus of claim 29, wherein the front surface iscurved.
 33. The apparatus of claim 31, wherein the front surface isconvexly curved.
 34. The apparatus of claim 32, wherein the frontsurface is convexly curved.
 35. The apparatus of claim 33, wherein thefirst tube is mounted to be longitudinally displaceable.
 36. Theapparatus of claim 34, wherein the first tube is mounted to belongitudinally displaceable.
 37. The apparatus of claim 35, wherein atleast two second tubes run concentrically to the first tube within thefirst tube, the second of the second tubes runnig at a distance to thelongitudinal axis of the first and the first of the second tubes. 38.The apparatus of claim 36, wherein at least two second tubes runconcentrically to the first tube within the first tube, the second ofthe second tubes runnig at a distance to the longitudinal axis of thefirst and the first of the second tubes.
 39. A process for manufacturingan optical fiber from a blank of starting material, the startingmaterial extruded through a vibrated nozzle.
 40. The process of claim39, wherein the virbation is in an ultrasonic range.
 41. A device forextruding an optical fiber from a blank of starting material,comprising: a ram that can be displaced longitudinally, and a nozzle,and a vibrator, coupled to the nozzle.
 42. The extrusion device of claim41, wherein the vibrator comprises a piezoelectric crystal.
 43. Theextrusion device of claim 42, wherein the blank of a firstcross-sectional shape and the nozzle has a second cross-sectional shapethat differs from the first cross sectional shape.
 44. The extrusiondevice of claim 43, wherein the blank has a circular cross sectionalshape and the nozzle has a square cross sectional shape.
 45. An opticalfiber for transmitting radiation, comprising: a fiber end characterizedby a reduced reflectivity microstructure.
 46. The optical fiber of claim45, wherein the microstructure is impressed on the fiber material. 47.The optical fiber of claim 46, wherein the microstructurescatters atleast a portion of the radiation emerging therefrom.
 48. The opticalfiber of claim 45, wherein the microstructure scatters at least aportion of the radiation emerging therefrom.
 49. The optical fiber ofclaim 48, wherein an element having the microstructure is affixed to theend of the fiber.
 50. The optical fiber of claim 45, wherein an elementhaving the microstructure is affixed to the end of the fiber.
 51. Theoptical fiber of claim 50, wherein the element is a radiation filterthat is transparent to certain wavelengths of the radiation.
 52. Theoptical fiber of claim 51, wherein the element is designed to bechemically resistant to substances that are present in its environment.53. The optical fiber of claim 52, wherein the element is an artificialdiamond.
 54. The optical fiber of claim 49, wherein the element is anartificial diamond.
 55. An optical fiber, comprising: a plurality oflight-conducting channels, the channels running internal to the fiber ina longitudinal direction, every channel capable of conducting lightthrough the fiber independent of the other channels.
 56. The opticalfiber of claim 55, wherein the channels are arranged in a matrix withrespect a cross-section of the fiber.
 57. The optical fiber of claim 56,wherein the channels are arranged in a rectangular matrix.
 58. Theoptical fiber of claim 57, wherein an outside cross-section of the fiberis angular.
 59. The optical fiber of claim 58, wherein the outside crosssection is rectangular.
 60. The optical fiber of claim 58, wherein theoutside cross section is square.
 61. A fiber bundle, comprising: aplurality of optical fibers, each said fiber having an angular outsidecross-sections; each said fiber comprising: a plurality oflight-conducting channels, the channels running internal to the fiber ina longitudinal direction, every channel capable of conducting lightthrough the fiber independent of the other channels.
 62. An opticalfiber, wherein the fiber comprises at least one light-conducting channelwith a rectangular, longitudinally-extending cross-section.